5 research outputs found

    变温超固相线液相烧结工艺对15Cr系高铬铸铁显微组织及性能的影响

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    为解决常规定温超固相线液相烧结出现的烧结温度窗口狭窄和产品力学性能对烧结温度波动敏感的问题,采用变温超固相线液相烧结工艺制备了粉末冶金高铬铸铁,研究了变温超固相线液相烧结的高温阶段工艺参数对15Cr系高铬铸铁显微组织和力学性能的影响,并与定温超固相线液相烧结制备的合金进行了对比。研究发现,变温超固相线液相烧结制备的合金由M7C3型碳化物、马氏体及少量奥氏体组成,通过高、低温两个阶段的烧结能够实现高效致密化和对显微组织的有效调控,制备出相对密度超过98.96%的高性能合金材料,烧结温度窗口相较于定温超固相线液相烧结扩展了15 ℃。在1225~1245 ℃、5~10 min的高温阶段窗口,随烧结温度升高与保温时间延长,合金显微组织逐渐粗化;当高温阶段烧结保温时间控制在10 min以内时,合金晶粒尺寸低于26.98 μm,组织粗化程度可接受。变温超固相线液相烧结高铬铸铁的硬度和冲击韧性优于定温超固相线液相烧结高铬铸铁,且冲击韧性在烧结窗口内保持稳定,平均值达12.10 J·cm−2。在1~3 J·cm−2冲击功下,变温超固相线液相烧结试样的抗冲击磨粒磨损性能优于定温超固相线液相烧结试样,随着冲击功提高,合金的抗冲击磨粒磨损性能提升从9.70%提高到19.83%

    Prediction of Energy Resolution in the JUNO Experiment

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    International audienceThis paper presents the energy resolution study in the JUNO experiment, incorporating the latest knowledge acquired during the detector construction phase. The determination of neutrino mass ordering in JUNO requires an exceptional energy resolution better than 3% at 1 MeV. To achieve this ambitious goal, significant efforts have been undertaken in the design and production of the key components of the JUNO detector. Various factors affecting the detection of inverse beta decay signals have an impact on the energy resolution, extending beyond the statistical fluctuations of the detected number of photons, such as the properties of liquid scintillator, performance of photomultiplier tubes, and the energy reconstruction algorithm. To account for these effects, a full JUNO simulation and reconstruction approach is employed. This enables the modeling of all relevant effects and the evaluation of associated inputs to accurately estimate the energy resolution. The study reveals an energy resolution of 2.95% at 1 MeV. Furthermore, the study assesses the contribution of major effects to the overall energy resolution budget. This analysis serves as a reference for interpreting future measurements of energy resolution during JUNO data taking. Moreover, it provides a guideline in comprehending the energy resolution characteristics of liquid scintillator-based detectors

    JUNO Sensitivity on Proton Decay pνˉK+p\to \bar\nu K^+ Searches

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    The Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this paper, the potential on searching for proton decay in pνˉK+p\to \bar\nu K^+ mode with JUNO is investigated.The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification. Moreover, the excellent energy resolution of JUNO permits to suppress the sizable background caused by other delayed signals. Based on these advantages, the detection efficiency for the proton decay via pνˉK+p\to \bar\nu K^+ is 36.9% with a background level of 0.2 events after 10 years of data taking. The estimated sensitivity based on 200 kton-years exposure is 9.6×10339.6 \times 10^{33} years, competitive with the current best limits on the proton lifetime in this channel

    JUNO sensitivity on proton decay p → ν K + searches*

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    The Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this study, the potential of searching for proton decay in the pνˉK+ p\to \bar{\nu} K^+ mode with JUNO is investigated. The kaon and its decay particles feature a clear three-fold coincidence signature that results in a high efficiency for identification. Moreover, the excellent energy resolution of JUNO permits suppression of the sizable background caused by other delayed signals. Based on these advantages, the detection efficiency for the proton decay via pνˉK+ p\to \bar{\nu} K^+ is 36.9% ± 4.9% with a background level of 0.2±0.05(syst)±0.2\pm 0.05({\rm syst})\pm 0.2(stat) 0.2({\rm stat}) events after 10 years of data collection. The estimated sensitivity based on 200 kton-years of exposure is 9.6×1033 9.6 \times 10^{33} years, which is competitive with the current best limits on the proton lifetime in this channel and complements the use of different detection technologies

    JUNO sensitivity on proton decay pνK+p → νK^{+} searches

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